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JPE - Sept09 - cover2-4.pmd - Pipes & Pipelines International ...

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160<br />

J, N/mm<br />

80<br />

60<br />

40<br />

20<br />

case (height = 3mm, length = 50mm, ligament =<br />

3mm), the following is observed based on results in<br />

Table 2:<br />

• increasing the height from 3 to 6 and 9mm<br />

leads to reductions in M of 3.8 and<br />

J2B E 0.5%<br />

5.5%, respectively;<br />

• increasing the ligament from 3 to 6 and<br />

9mm, leads to increases in M of 1.8<br />

J2B E 0.5%<br />

and 2.3%, respectively;<br />

• increasing the length from 50 to 100 and<br />

200mm leads to reductions in M of<br />

J2B E 0.5%<br />

1.1 and 1.8%, respectively.<br />

• The J-based limit loads for flaws located at a given<br />

ligament from the ID are nearly equal to those for<br />

flaws located at the same ligament from the OD (for<br />

example E1BH3L50L3M0 and E1BH3L50L14M0).<br />

• M J2B E (with J e based on the elastic pipe bending<br />

stress) is higher than M J2B EP (with J e based on the<br />

elastic-plastic pipe-bending stress) by approximately<br />

4%. This is not surprising since in the former case,<br />

for a given load level, the elastic driving force (J e ) and<br />

f(L r ) are higher, L r is lower, and M J is higher, see<br />

Equns 2 and 7.<br />

Comparison of flat-plate solutions<br />

with J-based solutions<br />

To facilitate comparison of the J-based limit loads with the<br />

codified flat-plate solutions reviewed earlier, the M J results<br />

The Journal of Pipeline Engineering<br />

OD=400mm, t=20mm, e=0.0mm. Embedded flaw near ID: 2a=3.0mm, 2c=50.0mm, pi=3mm, 'E1BH3L50L3M0'<br />

J estimate based on σ ref/σ M1 determined at 0.5% strain<br />

J max (FEA)<br />

J estimate based on M J2B EP 0.5% x (σ M1/σ M)<br />

J estimate based on M J2B EP 0.5%<br />

J estimate based on Global collapse,<br />

0<br />

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0<br />

Remote strain %<br />

Fig. 11. J results for model E1BH3L50L3M0 (from FEA and based on estimates of limit moment).<br />

(M J2B E 0.5% and M J2B EP 0.5% ) were expressed in terms of the<br />

non-dimensional parameter s ref /s M1 , where s M1 is the elasticplastic<br />

pipe-bending stress, and compared with s ref /s M1<br />

determined from the flat-plate solutions (as 1/n L ). The<br />

results are given in Table 3. The same results are reproduced<br />

as the ratio of s ref from the flat-plate solutions to s ref from<br />

M J2B EP 0.5% in Table 4. The following conclusions are drawn:<br />

Sample issue<br />

• s ref /s M1 estimates based on flat-plate solutions and<br />

local collapse with pin loading exceed significantly<br />

s ref /s M1 based on M J2B E 0.5% and M J2B EP 0.5% . Therefore,<br />

flat-plate solutions based on local collapse with pin<br />

loading lead to conservative assessments according<br />

to the following ranking (given in order of decreasing<br />

conservatism):<br />

• R6, local collapse, solution (b), pin loading<br />

(Equn 18)<br />

• BS 7910, local collapse, solution (a), pin<br />

loading (Equn 11)<br />

• R6, local collapse, solution (a), pin loading<br />

(Equn 15)<br />

• Table 4 shows that the BS 7910 flat-plate s ref solution<br />

exceeds s ref based on M J2B EP 0.5% by a margin which<br />

varies depending on flaw size and ligament. The<br />

margin is higher for deeper and longer flaws. Except<br />

for the shortest flaw considered (length = 25mm)<br />

and shallow flaws located near the middle of the<br />

thickness (height = 3mm and ligament >= 6mm) the<br />

margin exceeds 5%. These results apply to the<br />

stress-strain curve considered (low work hardening).

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